David Doll. Beyond SM theories Mark Wise paper BBU starting point and expansion Look at 2.24 and 2.26 to see difference between kinetic and pole scheme.

Slides:



Advertisements
Similar presentations
May 14, 2015Pavel Řezníček, IPNP Charles University, Prague1 Tests of ATLAS strip detector modules: beam, source, G4 simulations.
Advertisements

Detection of Gamma-Rays and Energetic Particles
Studies of the decay B  c K at the BaBar experiment Nick Barlow University of Manchester December 2003.
03 Aug NP041 KOPIO Experiment Measurement of K L    Hideki Morii (Kyoto Univ.) for the KOPIO collaborations Contents Physics Motivation.
Measurement of non BB Decays of Y(4S) to Y(1S)     and Y(2S)     Silvano Tosi Università & INFN Genova.
Owen Long, UC Santa Barbara Lake Louise Winter Institute, Feb Initial Performance of the BaBar Experiment Owen Long University of California, Santa.
David Doll 1. Outline Thesis topic: b →sγ Motivation Previous Analysis Babar overview Subdetector introduction and impact on thesis Previous work: Introduction.
16 May 2002Paul Dauncey - BaBar1 Measurements of CP asymmetries and branching fractions in B 0   +  ,  K +  ,  K + K  Paul Dauncey Imperial College,
Calorimetry and Showers Learning Objectives Understand the basic operation of a calorimeter (Measure the energy of a particle, and in the process, destroy.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
Ionization. Measuring Ions A beam of charged particles will ionize gas. –Particle energy E –Chamber area A An applied field will cause ions and electrons.
GlueX Simulations Status Report on CD3 geometry Richard Jones GlueX Collaboration Meeting, Newport News, January 10-12, 2008.
Preliminary Measurement of the BF(   → K -  0  ) using the B A B AR Detector Fabrizio Salvatore Royal Holloway University of London for the B A B AR.
Interaction of Particles with Matter
Chapter 22 Reflection and Refraction of Light 1. Dual nature of light 2. Geometric optics 3. Reflection and Refraction 4. Dispersion 5. Huygen’s Principle.
The LiC Detector Toy M. Valentan, M. Regler, R. Frühwirth Austrian Academy of Sciences Institute of High Energy Physics, Vienna InputSimulation ReconstructionOutput.
Recirculation Concept - Cyclotron Radio frequency alternating voltage Hollow metal drift tubes time t =0 time t =½ RF period D-shaped.
Charmonium Production at BaBar Jamie Boyd University of Bristol Photon 2003, Frascati 7 th -11 th April 2003 On behalf of the Collaboration.
The Number of Light Neutrino Families ● Physics motivation for measurement ● Direct / indirect searches for ● Analysis methodology for ● Single photon.
Lecture 1.3: Interaction of Radiation with Matter
Comparison of Endcap CID-PID Klaus Föhl PID meeting 27/3/2007 panda-meeting Genova Focussing Lightguides Time-of-Propagation Proximity Focussing.
NEW COMMENTS TO ILC BEAM ENERGY MEASUREMENTS BASED ON SYNCHROTRON RADIATION FROM MAGNETIC SPECTROMETER E.Syresin, B. Zalikhanov-DLNP, JINR R. Makarov-MSU.
Performance of the PANDA Barrel DIRC Prototype 1 GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt 2 Goethe-Universität Frankfurt Marko Zühlsdorf.
D 0 Measurement in Cu+Cu Collisions at √s=200GeV at STAR using the Silicon Inner Tracker (SVT+SSD) Sarah LaPointe Wayne State University For the STAR Collaboration.
The CLEO-c Detector Steve Gray Cornell University BESIII Workshop January 13, 2004.
Detectors (CLAS) Yarulin Rafael Department of Physics, Graduate School September 2003 Kyungpook National University.
Photodetection EDIT Internal photoelectric effect in Si Band gap (T=300K) = 1.12 eV (~1100 nm) More than 1 photoelectron can be created by light in silicon.
International Workshop on Linear Colliders, Geneve Muon reconstruction and identification in the ILD detector N. D’Ascenzo, V.Saveliev.
PSD Chip Calculations. Energy Conversions Erad Energy of incident radiation (MeV) evis Energy of visible photon radiation (eV) εcon Conversion efficiency.
2. RUTHERFORD BACKSCATTERING SPECTROMETRY Basic Principles.
Semiconductor detectors An introduction to semiconductor detector physics as applied to particle physics.
work for PID in Novosibirsk E.A.Kravchenko Budker INP, Novosibirsk.
1 Energy loss correction for a crystal calorimeter He Miao Institute of High Energy Physics Beijing, P.R.China.
Electron Detection for Compton Polarimetry Michael McDonald Outline -Compton Effect -Polarimetry -Detectors -Diamond Results.
Radiation Detectors In particular, Silicon Microstrip Detectors by Dr. Darrel Smith.
Tracking in High Density Environment
Lepton Flavor Violating  decays at B-factories: results and prospects Giovanni Marchiori Università di Pisa & I.N.F.N.
Silicon Detector Tracking ALCPG Workshop Cornell July 15, 2003 John Jaros.
03/21/2005Michael Spitznagel (MIT)Page 1 The Babar Drift Chamber Michael Spitznagel Massachusetts Institute of Technology.
Scan ~100 bar entry positions with laser diode measures transmitted intensity (relative to reference intensity) determine attenuation length (Λ) by aiming.
1 A CLUster COUnting Drift Chamber for ILC …and… can we adapt this chamber to SuperB ? F.Grancagnolo, INFN – Lecce, Italy.
The Babar Cherenkov Detector Detection of Internally Reflected Cherenkov Yuen-Jung Chang.
Radia Sia Syracuse Univ. 1 RICH 2004 Outline:  The CLEO-III RICH Detector  Physics Requirements  CLEO-III RICH at work… Performance of the CLEO-III.
Forward Tagger Simulations Implementation in GEMC Moller Shield Tracking Studies R. De Vita INFN –Genova Forward Tagger Meeting, CLAS12 Workshop, June.
TeV muons: from data handling to new physics phenomena Vladimir Palichik JINR, Dubna NEC’2009 Varna, September 07-14, 2009.
Measurements of B  X c l Decays Vera Lüth, SLAC BABAR Collaboration Inclusive BR (B  X c l ) and |V cb | Hadronic Mass Moments (Preliminary Measurement)
First results from SND at VEPP-2000 S. Serednyakov On behalf of SND group VIII International Workshop on e + e - Collisions from Phi to Psi, PHIPSI11,
Daniel Sherwood 03/2005 Search for Crypto-Exotic States in Babar Daniel Sherwood Dr. Liliana Teodorescu.
May 26-27, 2005Tadashi Nomura (Kyoto U), KRare05 at Frascati, Italy1 KOPIO Beam Catcher Tadashi Nomura (Kyoto U.) Contents –What is Beam Catcher? –Concept.
Data Analysis Practice looking for Φ(1020) Nuclear Physics Ⅲ Kyung-Eon,Choi.
Photon Transport Monte Carlo September 27, 2004 Matthew Jones/Riei IshizikiPurdue University Overview Physical processes PMT and electronics response Some.
The Collider Detector at Fermilab (aka CDF) Jennifer Pursley Intermediate Seminar Oct. 28, 2003.
P HOTON Y IELD DUE TO S CINTILLATION IN CF4 Bob Azmoun, Craig Woody ( BNL ) Nikolai Smirnov ( Yale University )
BESIII offline software group Status of BESIII Event Reconstruction System.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
View of TPC Optimization from Reconstruction Working Group Xin Qian and Tingjun Yang 1.
A Barrel DIRC using radiator plates AntiProton ANnihilations at DArmstadt Study of QCD with Antiprotons Charmonium Spectroscopy Search for Exotics Hadrons.
Particle Identification of the ALICE TPC via dE/dx
PhD thesis: Simulation & Reconstruction for the PANDA Barrel DIRC Official name: Open charm analysis tools Supervisor: Prof. Klaus Peters Maria Patsyuk.
Status of BESIII and upgrade of BESIII
“Performance test of a lead glass
Radio Coverage Prediction in Picocell Indoor Networks
Layout of Detectors for CLIC
CMS muon detectors and muon system performance
SuperB SVT Definition of sensor design and z-side connection scheme
Toy Monte Carlo for the Chromatic Correction in the Focusing DIRC Data
DE/dx Study at CEPC TPC An Fenfen
Study of e+e- pp process using initial state radiation with BaBar
Cluster Counting Drift Chamber as high precision tracker for ILC experiments G.F. Tassielli(1,2) (1) Dipartimento di Fisica dell’Universita’ del Salento,
Particles going through matter
Presentation transcript:

David Doll

Beyond SM theories

Mark Wise paper

BBU starting point and expansion Look at 2.24 and 2.26 to see difference between kinetic and pole scheme in hep-ph/

Former Analysis extended Novosibirsk function: Argus function: Source Babar doc where: m 0 is peak position, σ is width, τ is tail parameter Source Phys. Lett. B 241, 278 (1990) where a and b are parameters to be fit

Y(3S) and Such Properties Width = /- 2.5 MeV (hbar = 6.58 x 10^-16 eVs) Liftime = 3.2 x 10 ^-23 s BBbar decay > 96% of the time (PDG)

SVT Extended Best angular information comes from inner points, not subject to multiple scattering. Particles with p_t less than 100MeV/c don’t make the drift chamber, and only with p_t > 120 MeV/c is the drift chamber reliable. Goal of 70% eff. In tracking information for MeV/c particles Coverage is between 20.1 and degrees. 5 Layers, double sided, inside (junction side) measures z, outside measures phi for first 3 layers, opposite for last 2. ~150,000 channels Inner 3 layers for measuring impact parameters, outer two for pattern recognition and low p_t tracking.

SVT Extended dE/dx formula for charged particles (from infn): Bethe-Bloch formula MC simulation of SVT (source Babar doc).

DCH Extended AUVAUVAUVA arrangement of the superlayers (10), each consisting of 4 layers. Axial (A) and stereo (U,V) 1.08%X0 at normal incidence dE/dx from ionization loss

DIRC extended Cherenkov Angle relation: Forward end has a mirror to reflect forward propagating photons Index of refraction for fused silica = 1.473

EMC extended 15.8 to o polar angle coverage (90% CM coverage) Energy resolution described empirically by: where a represents fluctuations in photon statistics and electronic noise, and b, constant term, comes from non-uniformity in light collection, influence of material in front, and calibration uncertainty Ultimately, a = 2.32% and b = 1.85% Radiation length, corresponding to the length for an electron to drop to 1/e it’s energy, or 7/9 the mean free path for pair production of a photon.

EMC Extended Source photon for low energy calibration from the process: 19 F + n → 16 N + α, 16 N → 16 O* + β, 16 O* → 16 O + γ

IFR Extended 21 active detector layers in the barrel, 18 in the endcaps Bakelite sheet bulk resistivity is 10^11 – 10^12 ohm cm Gas: 56.7% Argon, 38.8% Freon 134a, and 4.5% isobutane Graphite surfaces connected to ~8kV and ground.

IFR Extended LST

Punzi FOM extended